Lagrangian of a disk with a hole on an inclined plane

In summary: The component of the angular momentum in the direction of the axle is conserved. So we can rename the coordinate system to have the axle in the z-direction and the component of the angular momentum in this direction is L_z=Iω. The kinetic energy is T=1/2(m+M)v^2+1/2Iω^2, where v is the velocity of the center of mass of the disk. You can eliminate v^2 using the equation for the constraint v=ωr. For the potential energy, it might be easier to work in a coordinate system which rotates with the disk around the axle.
  • #1
Physgeek64
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11

Homework Statement


A wheel consists of a circular uniform disk with a circular hole in it. The disc is
of radius R and mass per unit area ρ. The hole is of radius ro and an axle of radius ro
passes through it. The centre of the hole is offset radially from the centre of the disk by
ro. The wheel rotates without friction about the axle. Using the parallel axis theorem,
or otherwise, evaluate an expression for the moment of inertia of the wheel around the
axle. The angular speed of the wheel is ω, what is its kinetic energy?

The wheel is removed from the axle and rolls without slipping along a flat surface with the same angular speed. Show that its rotational kinetic energy is less than for the case of rotation about the axle

The wheel is placed on a surface sloping at an angle α where it rolls without slipping. It starts from rest with the centre of the hole directly above the centre of the disk. Neglecting the contribution of the hole to kinetic energy, use the Euler Lagrange method to find the equation of motion

Homework Equations


L=T-V
KE of rotation= 1/2*I*(ω)^2

(Most are below)

The Attempt at a Solution


So I think I've done the first two parts okay- I got the the moment of inertia for the first part to be 1/2*pi*rho*(R^4+R^2*r^2-r^4) and the KE to be half that times the ω^2

For the next part I for the KE to be 1/2*pi*rho*ω^2*(R^4-3r^4), and showed that the condition for the KE to be less is R>sqrt(2)r, which is obviously satisfied by the geometry of the system

For the last part, I am a bit confused because the centre of mass does not move with in a straight path, and is rotating

So I first found the location of the COM relative to the centre of the disc, and got this to be -r^3/(R^2-r^2)

So the rational KE of the COM is 1/2*((pi*rho)*(r^6)*ω^2)/((R^2-r^2) (sorry- I am still not sure how to use latex properly! I will be practicing, so please bare with me) Also- Here ω is varying- but I thought this would be neater to write than 'theta dot'

The rotational KE of the disc, ignoring the hole is

1/4*(pi*rho)*ω^2*R^4

But then I am not sure what the translational KE of the disc is since the COM is moving downwards and rotating, so its translational KE is modulating. I'm not sure if the question permits me to simply ignore the hole completely and simply use the rational KE of the disc as if it were solid, and the translational KE of the COM as if the disc were solid. If so then I think I can almost do this question.
And similarly, for the PE since the height is moving downwards, but periodically varying as it rotates I'm struggling to see how to formulate it

Edit:
So far for the potential energy I have

PE= -M*g*s*sin(alpha) - Mg*(centre off mass position)*sin(theta), where theta is the integral of ω and M=pi*rho*(R^2-r^2),
but I am not sure if this is correct?
Thanks in advance :)
 
Last edited:
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  • #2
Physgeek64 said:
So the rational KE of the COM is 1/2*((pi*rho)*(r^6)*ω^2)/((R^2-r^2)
I don't see how you got this (would it vanish for r->0?) and I also don't think it is necessary. It is easier to work in the frame of the geometric center of the disk.
 

Related to Lagrangian of a disk with a hole on an inclined plane

1. What is the Lagrangian of a disk with a hole on an inclined plane?

The Lagrangian of a disk with a hole on an inclined plane is a mathematical expression that describes the energy of the system. It takes into account the kinetic energy, potential energy, and any external forces acting on the disk. It is typically represented as L = T - V, where T is the kinetic energy and V is the potential energy.

2. How is the Lagrangian derived for this system?

The Lagrangian for a disk with a hole on an inclined plane is derived using the principles of Lagrangian mechanics. This involves using the Euler-Lagrange equations to find the partial derivatives of the Lagrangian with respect to the position and velocity variables of the system. These equations can then be solved to obtain the final expression for the Lagrangian.

3. What factors affect the Lagrangian of this system?

The Lagrangian of a disk with a hole on an inclined plane is affected by several factors, including the mass and shape of the disk, the angle of inclination of the plane, and any external forces acting on the disk. It can also be influenced by the presence of friction or other non-conservative forces.

4. How is the Lagrangian used to analyze the motion of this system?

The Lagrangian is used to derive the equations of motion for the system, which describe how the position and velocity of the disk change over time. These equations can then be solved to determine the trajectory and other characteristics of the disk's motion, such as its angular velocity and acceleration.

5. Can the Lagrangian be used to analyze other systems besides a disk with a hole on an inclined plane?

Yes, the Lagrangian can be used to analyze a wide range of physical systems, including those with multiple objects, constraints, and degrees of freedom. It is a powerful tool in classical mechanics and is often used to study the motion of particles, rigid bodies, and more complex systems.

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